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Chaiwoot Boonyasiriwat

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1 Chaiwoot Boonyasiriwat
3D Multisource Full-Waveform Inversion using Quasi-Monte Carlo Phase Encoding Chaiwoot Boonyasiriwat Jan. 7, 2010

2 Outline Introduction to Multisource Technology Phase Encoding
Multisource Full-Waveform Inversion Quasi-Monte Carlo Phase Encoding Numerical Results 3D SEG/EAGE Overthrust Model Summary Future Work Acknowledgment 1

3 Introduction: Multisource Tech.
Migration Delayed-shot migration (Zhang et al., 2005) Random phase encoding (Romero et al., 2000) Plane-wave migration (Liu et al., 2006; Shan and Biondi, 2008; Shan et al., 2009) Full-Waveform Inversion (FWI) Plane-wave FWI (Vigh and Starr, 2008) Random phase encoding (Krebs et al., 2009; Zhan et al., 2009) 2

4 Single-Source Method 3

5 Linear Phase Encoding—Planewave Decomposition
Multisource Method Linear Phase Encoding—Planewave Decomposition 4

6 Multisource Method Random Phase Encoding 5

7 CSG vs SSG CSG SSG 6

8 Outline Introduction to Multisource Technology Phase Encoding
Multisource Full-Waveform Inversion Quasi-Monte Carlo Phase Encoding Numerical Results 3D SEG/EAGE Overthrust Model Summary Future Work Acknowledgment 7

9 Evaluate misfit function and compute gradient
Conventional FWI Model No Observed Data Evaluate misfit function and compute gradient Evaluate misfit function Perturb Model No Search criterion Convergence criterion Yes Done Yes 8

10 Evaluate misfit function and compute gradient
Multisource FWI Model No Encoded Data Evaluate misfit function and compute gradient Evaluate misfit function Perturb Model No Search criterion Convergence criterion Yes Done Yes 9

11 2D Multisource FWI Krebs Method (ExxonMobil): one SSG,
random source polarity, dynamic encoding 8

12 2D Multisource FWI Zhan Method (UTAM): multiple SSGs,
random time shift, static encoding, deblurring filter 9

13 Krebs Source Configuration
3D Multisource FWI Krebs Source Configuration 10

14 Closely Packed Source Configuration
3D Multisource FWI Closely Packed Source Configuration 11

15 Loosely Packed Source Configuration
3D Multisource FWI Loosely Packed Source Configuration 12

16 Quasi-Monte Carlo Source Configuration
3D Multisource FWI Quasi-Monte Carlo Source Configuration 13

17 Static vs Dynamic Configuration
Iteration 1 2 14

18 Outline Introduction to Multisource Technology Phase Encoding
Multisource Full-Waveform Inversion Quasi-Monte Carlo Phase Encoding Numerical Results 3D SEG/EAGE Overthrust Model Summary Future Work Acknowledgment 15

19 3D SEG/EAGE Overthrust Model
16

20 Numerical Results True Velocity Model 17

21 Initial Velocity Model
Numerical Results Initial Velocity Model 18

22 Velocity Model from Static QMC
Numerical Results Velocity Model from Static QMC 19

23 Velocity Model from Dynamic QMC
Numerical Results Velocity Model from Dynamic QMC 20

24 Velocity Model from Krebs Method
Numerical Results Velocity Model from Krebs Method 21

25 Outline Introduction to Multisource Technology
Multisource Full-Waveform Inversion Numerical Results 3D SEG/EAGE Overthrust Model Summary Future Work Acknowledgment 22

26 Summary 3D multisource FWI using multiple SSGs is compared with multisource FWI using one SSG. Using multiple SSGs and a dynamic QMC phase encoding provides a better-quality velocity model than a static QMC phase encoding and Krebs method. Theoretical speedups need to be verified. More reliable timing results will be presented later. 23

27 Outline Introduction to Multisource Technology
Multisource Full-Waveform Inversion Numerical Results 3D SEG/EAGE Overthrust Model Summary Future Work Acknowledgment 24

28 Future Work Compare various multisource configurations.
Compare random phase encoding with plane-wave encoding. Apply random time shifts and deblurring filter. Apply 3D multisource FWI to field data. 25

29 Acknowledgment Sponsors of 2009 UTAM consortium
HPC: Aron Ahmadia and Mark Cheeseman Shaheen: Iain Georgeson and Jonathan Anderson Multisource: Ge Zhan and Wei Dai Workstation: Benoit Marchand KAUST: Jerry Schuster 26


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